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Question: Work done in vaporization of one mole of water at 373K against the pressure of 1atm is approximately...

Work done in vaporization of one mole of water at 373K against the pressure of 1atm is approximately :
A.3100J\, - 3100J\,
B.31.20J\, - 31.20J\,
C.20.2J\, - 20.2J\,
D.+3100J\, + 3100J\,

Explanation

Solution

In thermodynamics, there is no work in a system, and work is an operation performed by or on a system. Gases can work against continuous exterior pressure by expansion or compression. Gas work is often also called pressure-volume or PV\,PV\, work.
Formula used:
PV=nRTPV = nRT\,
Where, P=\,P = \,Pressure
V=\,V = \,Volume
n=\,n = \,number of moles
R=\,R = \,Universal gas constant
T=\,T = \,absolute temperature
W=Pext×ΔV\,W = - {P_{ext}} \times \Delta V
Where W=\,W = \,Work
Pext=\,{P_{ext}} = \,External Pressure
ΔV=\,\Delta V = \,Change in volume

Complete step by step solution:
Let us first calculate volume of water before vaporization;
V=mdV = \dfrac{m}{d}\,
Where, V=\,V = \,volume, m=\,m = \,mass and d=\,d = \,density
Here, we have one mole of water which is equal to 18g\,18g\,
Therefore, V=18g1g/ml\,V = \dfrac{{18g}}{{1g/ml}}\,
As the density of one mole of water is equal to 1g/ml\,1g/ml\,at 373K\,373K\,
Therefore by solving the equation we get, V1=18ml=0.018l\,{V_1} = 18ml\, = 0.018l\,
Now, let’s calculate V2\,{V_2}\, which is the volume of water after vaporization;
PV2=nRTP{V_2} = nRT\,
Where, P=\,P = \, Pressure
V2=\,{V_2} = \, Volume after vaporization
n=\,n = \, number of moles
R=\,R = \, Universal gas constant
T=\,T = \, absolute temperature
From this we get;
V2=nRTP\,{V_2} = \dfrac{{nRT}}{P}\, as per ideal gas equation mentioned above
n=1,R=0.0821L.atm/mol.K,T=373K,P=1atm\,n = 1,\,R = 0.0821L.atm/mol.K,\,T = 373K,P = 1atm\,
Substituting them in the equation we get;
1×0.0821×3731=30.6l\, \Rightarrow \dfrac{{1 \times 0.0821 \times 373}}{1} = 30.6l\,
Here V1\,{V_1}\, is negligible with respect to V2\,{V_2}\,, So we can ignore V1\,{V_1}\,and therefore, ΔV=30.6l\,\Delta V = 30.6l\,
Now, let us calculate the work done here,
W=Pext×ΔVW = - {P_{ext}} \times \Delta V\,
Where W=\,W = \,Work
Pext=\,{P_{ext}} = \,External Pressure
ΔV=\,\Delta V = \,Change in volume

Here, by converting the unit of volume and pressure we get;
ΔV=30.6l=30.6×103m3\,\Delta V = 30.6l = 30.6 \times {10^{ - 3}}{m^3}\,and P=1atm=101325Pascal\,P = 1atm = 101325Pascal\,
Therefore, W=101325×30.6×103\,W = \, - 101325 \times 30.6 \times {10^{ - 3}}\,
=3100J\, = - 3100J\,
Here, a negative sign shows that work is done by the system.
So, for this question option A is the correct answer.

Note:
Work done by a system in thermodynamics is the energy transmitted by the system to its surroundings by a process by which the system can exert macroscopic forces on its surroundings naturally, where those forces and their external effects can be calculated. So, in sign conventions, the energy transmitted here is represented as negative work done by the system on its surroundings.